supplementary materials


bt2515 scheme

Acta Cryst. (2007). E63, m2886    [ doi:10.1107/S160053680704620X ]

Bis{[mu]-1,4-bis[(diphenylphosphanyl)ethynyl]benzene-[kappa]2P:P'}bis[trans-diiodidopalladium(II)] chloroform trisolvate

W. Y. Chan, T. Baumgartner, A. J. Lough and I. Manners

Abstract top

The title compound, [Pd2I4(C34H24P2)2]·3CHCl3, was obtained from the direct reaction of PdI2 with 1,4-bis[(diphenylphosphanyl)ethynyl]benzene. The dimer complex molecule is centrosymmetric, with each PdII atom in a slightly distorted square-planar coordination geometry.

Comment top

The bidentate phosphane ligand used in this work has been previously found to form a triangle when reacted with PtCl2 (Baumgartner et al., 2002). In this work, we report the formation of a rectangle using PdI2 as the metal source. The Pd centres in the title compound exhibit a slightly distorted square planar geometry, where the P—Pd—I angles deviate from 90° by less than 3°.

Related literature top

Metal-containing rings are currently of interest as polymer precursors (Nguyen et al., 1999; Herbert et al., 2007). We have also determined the structure of a triclinic modification of the title compound (Baumgartner et al., 2007). A related complex containing PtII atoms and chloride ligands was found to form a triangle (Baumgartner et al., 2002).

Experimental top

PdI2 (11 mg, 0.031 mmol) and 1,4-bis-[(diphenylphosphanyl)-ethynyl]-benzene (15 mg, 0.030 mmol) was added to CDCl3 (0.6 ml). Crystals of the title compound was obtained after 2 days.

Refinement top

All hydrogen atoms were placed in calculated positions with C—H = 0.95 or 1.00 Å and were included in the refinement in the riding-motion approximation with Uiso(H) = 1.2Ueq(C). One of the CHCl3 solvent molecules is disordered over a twofold rotation axis. For each CHCl3 the three C—Cl distances were constrained to be equal with a standard uncertainty of 0.002Å [see: SADI command in SHELXTL (Sheldrick, 2001)]

Computing details top

Data collection: COLLECT (Nonius, 2002); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN (Otwinowski & Minor, 1997); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXTL (Sheldrick, 2001); molecular graphics: SHELXTL (Sheldrick, 2001); software used to prepare material for publication: SHELXTL (Sheldrick, 2001).

Figures top
[Figure 1] Fig. 1. The molecular structure with displacement ellipsoids drawn at the 30% probability level. Neither the chloroform solvent molecules nor H atoms are shown. Atoms labeled with the suffix 'a' are related by the symmetry operator (−x + 3/2,-y + 1/2,-z + 1).
Bis{µ-1,4-bis[(diphenylphosphanyl)ethynyl]benzene-κ2P:P'}bis[trans- diiodidopalladium(II)] chloroform trisolvate top
Crystal data top
[Pd2I4(C34H24P2)2]·3CHCl3F000 = 3976
Mr = 2067.45Dx = 1.790 Mg m3
Monoclinic, C2/cMo Kα radiation
λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 19576 reflections
a = 20.8960 (9) Åθ = 2.6–25.0º
b = 9.5920 (5) ŵ = 2.52 mm1
c = 38.832 (2) ÅT = 150 (1) K
β = 99.804 (3)ºNeedle, colourless
V = 7669.6 (7) Å30.14 × 0.06 × 0.02 mm
Z = 4
Data collection top
Nonius KappaCCD
diffractometer
6672 independent reflections
Radiation source: fine-focus sealed tube3732 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.086
Detector resolution: 9 pixels mm-1θmax = 25.0º
T = 150(2) Kθmin = 2.6º
φ scans and ω scans with κ offsetsh = 24→24
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
k = 11→11
Tmin = 0.827, Tmax = 0.958l = 45→46
19576 measured reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.056H-atom parameters constrained
wR(F2) = 0.112  w = 1/[σ2(Fo2) + (0.024P)2 + 42.7375P]
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max = 0.002
6672 reflectionsΔρmax = 1.06 e Å3
411 parametersΔρmin = 0.91 e Å3
4 restraintsExtinction correction: none
Primary atom site location: structure-invariant direct methods
Crystal data top
[Pd2I4(C34H24P2)2]·3CHCl3V = 7669.6 (7) Å3
Mr = 2067.45Z = 4
Monoclinic, C2/cMo Kα
a = 20.8960 (9) ŵ = 2.52 mm1
b = 9.5920 (5) ÅT = 150 (1) K
c = 38.832 (2) Å0.14 × 0.06 × 0.02 mm
β = 99.804 (3)º
Data collection top
Nonius KappaCCD
diffractometer
6672 independent reflections
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
3732 reflections with I > 2σ(I)
Tmin = 0.827, Tmax = 0.958Rint = 0.086
19576 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0564 restraints
wR(F2) = 0.112H-atom parameters constrained
S = 1.01  w = 1/[σ2(Fo2) + (0.024P)2 + 42.7375P]
where P = (Fo2 + 2Fc2)/3
6672 reflectionsΔρmax = 1.06 e Å3
411 parametersΔρmin = 0.91 e Å3
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Pd10.67135 (3)0.12571 (7)0.633756 (18)0.0337 (2)
I10.72848 (3)0.04250 (7)0.595490 (18)0.0489 (2)
I20.61881 (3)0.24764 (6)0.681462 (16)0.04193 (19)
P10.57291 (10)0.0364 (2)0.60639 (6)0.0338 (6)
P20.77171 (11)0.2254 (2)0.65447 (6)0.0363 (6)
C10.5693 (4)0.0548 (9)0.5615 (3)0.044 (3)
C20.5810 (4)0.0764 (9)0.5327 (2)0.040 (2)
C30.6019 (4)0.1060 (10)0.5002 (2)0.040 (2)
C40.6216 (5)0.2398 (11)0.4932 (3)0.061 (3)
H4A0.61920.31230.50960.073*
C50.6448 (5)0.2686 (11)0.4626 (3)0.059 (3)
H5A0.65770.36080.45800.071*
C60.6491 (4)0.1649 (10)0.4388 (2)0.043 (2)
C70.6299 (4)0.0311 (9)0.4456 (2)0.043 (2)
H7A0.63290.04110.42910.051*
C80.6064 (4)0.0008 (10)0.4760 (2)0.043 (2)
H8A0.59330.09150.48030.052*
C90.6710 (4)0.1963 (9)0.4067 (3)0.045 (3)
C100.6902 (4)0.2313 (9)0.3808 (2)0.039 (2)
C110.5605 (4)0.1473 (9)0.6139 (2)0.034 (2)
C120.5926 (4)0.2073 (10)0.6446 (2)0.045 (3)
H12A0.62270.15410.66040.054*
C130.5805 (4)0.3451 (10)0.6522 (3)0.047 (3)
H13A0.60240.38670.67310.056*
C140.5369 (5)0.4205 (10)0.6294 (3)0.053 (3)
H14A0.52830.51450.63480.063*
C150.5047 (5)0.3619 (11)0.5983 (3)0.064 (3)
H15A0.47450.41550.58260.077*
C160.5172 (4)0.2262 (9)0.5908 (3)0.044 (3)
H16A0.49600.18580.56950.053*
C210.4980 (4)0.1166 (9)0.6141 (2)0.034 (2)
C220.4672 (4)0.0657 (10)0.6404 (2)0.045 (3)
H22A0.48460.01300.65360.054*
C230.4114 (4)0.1278 (11)0.6476 (3)0.051 (3)
H23A0.39040.09110.66550.061*
C240.3862 (5)0.2435 (11)0.6288 (3)0.061 (3)
H24A0.34790.28640.63390.073*
C250.4161 (4)0.2965 (9)0.6030 (3)0.057 (3)
H25A0.39880.37630.59030.069*
C260.4718 (4)0.2337 (9)0.5956 (2)0.045 (2)
H26A0.49240.27080.57760.053*
C310.7750 (4)0.3889 (10)0.6778 (3)0.041 (2)
C320.8069 (5)0.4039 (11)0.7117 (3)0.055 (3)
H32A0.82680.32490.72380.066*
C330.8103 (5)0.5302 (14)0.7282 (3)0.076 (4)
H33A0.83240.53860.75170.092*
C340.7823 (5)0.6428 (14)0.7111 (4)0.080 (4)
H34A0.78430.72970.72300.096*
C350.7511 (5)0.6362 (12)0.6771 (4)0.068 (4)
H35A0.73210.71680.66540.082*
C360.7483 (4)0.5061 (11)0.6601 (3)0.053 (3)
H36A0.72790.49880.63640.063*
C410.8270 (4)0.1125 (9)0.6827 (2)0.038 (2)
C420.8062 (5)0.0596 (10)0.7121 (3)0.056 (3)
H42A0.76330.07720.71600.067*
C430.8482 (6)0.0186 (11)0.7354 (3)0.067 (3)
H43A0.83430.05080.75610.080*
C440.9086 (6)0.0514 (11)0.7300 (3)0.071 (3)
H44A0.93640.10860.74610.085*
C450.9286 (5)0.0010 (11)0.7005 (3)0.066 (3)
H45A0.97100.02050.69630.080*
C460.8881 (5)0.0846 (10)0.6767 (3)0.053 (3)
H46A0.90290.12140.65670.064*
Cl10.56608 (16)0.6246 (3)0.51296 (10)0.0983 (11)
Cl20.7013 (2)0.6345 (6)0.5168 (2)0.255 (4)
Cl30.6484 (3)0.4900 (7)0.56931 (13)0.206 (3)
C1S0.63949 (19)0.6309 (12)0.5412 (2)0.150 (8)
H1SA0.64120.71850.55530.180*
Cl51.03790 (18)0.6728 (4)0.72255 (9)0.1068 (12)
Cl41.00000.4169 (5)0.75000.125 (2)
C2S0.9795 (9)0.5888 (12)0.7413 (6)0.110 (13)0.50
H2SA0.94040.58880.72420.132*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pd10.0336 (4)0.0372 (4)0.0304 (4)0.0009 (3)0.0059 (3)0.0015 (4)
I10.0401 (4)0.0537 (4)0.0545 (5)0.0011 (3)0.0122 (3)0.0148 (4)
I20.0428 (4)0.0494 (4)0.0349 (4)0.0031 (3)0.0102 (3)0.0075 (3)
P10.0339 (13)0.0402 (15)0.0282 (15)0.0027 (11)0.0075 (11)0.0005 (12)
P20.0398 (14)0.0423 (16)0.0275 (14)0.0021 (12)0.0076 (12)0.0013 (12)
C10.045 (6)0.042 (6)0.048 (7)0.003 (5)0.015 (5)0.009 (5)
C20.043 (6)0.041 (6)0.037 (6)0.012 (5)0.009 (5)0.003 (5)
C30.051 (6)0.044 (6)0.027 (6)0.006 (5)0.012 (5)0.001 (5)
C40.101 (9)0.050 (7)0.036 (7)0.014 (6)0.024 (6)0.004 (5)
C50.081 (8)0.058 (7)0.044 (7)0.025 (6)0.023 (6)0.002 (6)
C60.050 (6)0.044 (6)0.036 (6)0.009 (5)0.009 (5)0.001 (5)
C70.051 (6)0.044 (6)0.033 (6)0.014 (5)0.009 (5)0.001 (5)
C80.047 (6)0.045 (6)0.038 (6)0.008 (5)0.010 (5)0.007 (5)
C90.039 (6)0.051 (6)0.045 (7)0.012 (5)0.009 (5)0.006 (5)
C100.037 (5)0.040 (6)0.042 (6)0.016 (5)0.010 (5)0.001 (5)
C110.032 (5)0.041 (6)0.033 (6)0.002 (5)0.012 (5)0.003 (5)
C120.054 (6)0.048 (7)0.036 (7)0.011 (5)0.012 (5)0.000 (5)
C130.038 (6)0.047 (7)0.052 (7)0.000 (5)0.002 (5)0.004 (6)
C140.062 (7)0.033 (6)0.065 (8)0.005 (5)0.018 (6)0.012 (6)
C150.068 (7)0.043 (7)0.079 (10)0.021 (6)0.007 (7)0.009 (7)
C160.043 (6)0.033 (6)0.054 (7)0.009 (5)0.000 (5)0.001 (5)
C210.034 (5)0.034 (6)0.035 (6)0.000 (4)0.006 (5)0.001 (5)
C220.045 (6)0.055 (6)0.040 (6)0.002 (5)0.023 (5)0.004 (5)
C230.050 (6)0.060 (7)0.043 (7)0.003 (6)0.009 (5)0.005 (6)
C240.038 (6)0.056 (7)0.089 (9)0.005 (6)0.012 (6)0.018 (7)
C250.035 (6)0.034 (6)0.102 (10)0.006 (5)0.006 (6)0.006 (6)
C260.044 (6)0.039 (6)0.051 (7)0.009 (5)0.010 (5)0.001 (5)
C310.040 (6)0.054 (7)0.029 (6)0.014 (5)0.003 (5)0.001 (5)
C320.059 (7)0.048 (7)0.061 (8)0.000 (5)0.017 (6)0.014 (6)
C330.067 (8)0.091 (10)0.071 (10)0.005 (8)0.012 (7)0.029 (9)
C340.047 (8)0.072 (10)0.126 (14)0.017 (7)0.026 (8)0.049 (10)
C350.047 (7)0.052 (8)0.111 (12)0.007 (6)0.025 (8)0.002 (8)
C360.046 (6)0.053 (7)0.059 (8)0.011 (6)0.006 (6)0.001 (6)
C410.036 (5)0.039 (6)0.037 (6)0.001 (5)0.001 (5)0.001 (5)
C420.052 (6)0.064 (7)0.049 (7)0.005 (6)0.004 (6)0.024 (6)
C430.071 (8)0.064 (8)0.056 (8)0.009 (7)0.017 (7)0.032 (6)
C440.064 (8)0.058 (8)0.080 (10)0.004 (7)0.021 (7)0.023 (7)
C450.050 (7)0.074 (9)0.073 (9)0.026 (6)0.005 (7)0.000 (7)
C460.049 (6)0.062 (7)0.048 (7)0.008 (6)0.005 (6)0.002 (6)
Cl10.106 (3)0.084 (2)0.103 (3)0.009 (2)0.012 (2)0.011 (2)
Cl20.114 (4)0.210 (6)0.467 (11)0.044 (4)0.127 (5)0.152 (7)
Cl30.205 (5)0.282 (7)0.101 (4)0.136 (5)0.064 (4)0.085 (4)
C1S0.059 (9)0.165 (16)0.21 (2)0.002 (10)0.009 (11)0.137 (15)
Cl50.127 (3)0.115 (3)0.084 (3)0.009 (2)0.033 (2)0.017 (2)
Cl40.150 (5)0.084 (4)0.159 (6)0.0000.081 (4)0.000
C2S0.042 (18)0.12 (2)0.18 (4)0.011 (13)0.05 (2)0.10 (2)
Geometric parameters (Å, °) top
Pd1—P12.313 (2)C23—C241.383 (13)
Pd1—P22.321 (2)C23—H23A0.9500
Pd1—I22.5880 (9)C24—C251.365 (13)
Pd1—I12.6155 (9)C24—H24A0.9500
P1—C11.743 (10)C25—C261.384 (11)
P1—C111.812 (9)C25—H25A0.9500
P1—C211.813 (8)C26—H26A0.9500
P2—C10i1.749 (9)C31—C321.379 (12)
P2—C311.806 (10)C31—C361.384 (12)
P2—C411.809 (9)C32—C331.367 (13)
C1—C21.202 (11)C32—H32A0.9500
C2—C31.434 (12)C33—C341.349 (16)
C3—C41.388 (12)C33—H33A0.9500
C3—C81.393 (11)C34—C351.370 (15)
C4—C51.388 (12)C34—H34A0.9500
C4—H4A0.9500C35—C361.408 (13)
C5—C61.371 (12)C35—H35A0.9500
C5—H5A0.9500C36—H36A0.9500
C6—C71.384 (11)C41—C461.364 (11)
C6—C91.430 (12)C41—C421.386 (12)
C7—C81.384 (11)C42—C431.373 (12)
C7—H7A0.9500C42—H42A0.9500
C8—H8A0.9500C43—C441.351 (13)
C9—C101.191 (11)C43—H43A0.9500
C10—P2i1.749 (9)C44—C451.381 (14)
C11—C161.386 (11)C44—H44A0.9500
C11—C121.390 (11)C45—C461.396 (13)
C12—C131.386 (12)C45—H45A0.9500
C12—H12A0.9500C46—H46A0.9500
C13—C141.363 (12)Cl1—C1S1.728 (5)
C13—H13A0.9500Cl2—C1S1.728 (5)
C14—C151.396 (13)Cl3—C1S1.728 (5)
C14—H14A0.9500C1S—H1SA1.0000
C15—C161.370 (12)Cl5—C2Sii1.71 (2)
C15—H15A0.9500Cl5—C2S1.723 (11)
C16—H16A0.9500Cl4—C2S1.723 (11)
C21—C221.384 (11)Cl4—C2Sii1.723 (11)
C21—C261.395 (11)C2S—C2Sii1.00 (4)
C22—C231.379 (11)C2S—Cl5ii1.71 (2)
C22—H22A0.9500C2S—H2SA0.9600
P1—Pd1—P2172.93 (9)C22—C23—H23A120.1
P1—Pd1—I292.51 (6)C24—C23—H23A120.1
P2—Pd1—I291.96 (6)C25—C24—C23120.3 (9)
P1—Pd1—I188.09 (6)C25—C24—H24A119.8
P2—Pd1—I188.75 (6)C23—C24—H24A119.8
I2—Pd1—I1167.36 (4)C24—C25—C26119.9 (10)
C1—P1—C11106.1 (4)C24—C25—H25A120.1
C1—P1—C21103.4 (4)C26—C25—H25A120.1
C11—P1—C21103.6 (4)C25—C26—C21120.8 (9)
C1—P1—Pd1107.8 (3)C25—C26—H26A119.6
C11—P1—Pd1115.3 (3)C21—C26—H26A119.6
C21—P1—Pd1119.5 (3)C32—C31—C36118.5 (10)
C10i—P2—C31101.7 (4)C32—C31—P2122.7 (8)
C10i—P2—C41106.7 (4)C36—C31—P2118.6 (8)
C31—P2—C41104.5 (4)C33—C32—C31121.3 (11)
C10i—P2—Pd1109.3 (3)C33—C32—H32A119.4
C31—P2—Pd1119.1 (3)C31—C32—H32A119.4
C41—P2—Pd1114.2 (3)C34—C33—C32119.6 (12)
C2—C1—P1165.4 (9)C34—C33—H33A120.2
C1—C2—C3173.7 (10)C32—C33—H33A120.2
C4—C3—C8118.9 (8)C33—C34—C35122.2 (13)
C4—C3—C2120.0 (8)C33—C34—H34A118.9
C8—C3—C2121.1 (8)C35—C34—H34A118.9
C3—C4—C5120.6 (9)C34—C35—C36117.9 (12)
C3—C4—H4A119.7C34—C35—H35A121.0
C5—C4—H4A119.7C36—C35—H35A121.0
C6—C5—C4120.4 (9)C31—C36—C35120.4 (10)
C6—C5—H5A119.8C31—C36—H36A119.8
C4—C5—H5A119.8C35—C36—H36A119.8
C5—C6—C7119.3 (9)C46—C41—C42120.2 (9)
C5—C6—C9120.1 (9)C46—C41—P2122.3 (7)
C7—C6—C9120.5 (9)C42—C41—P2117.4 (7)
C6—C7—C8120.9 (9)C43—C42—C41119.3 (10)
C6—C7—H7A119.5C43—C42—H42A120.3
C8—C7—H7A119.5C41—C42—H42A120.3
C7—C8—C3119.8 (8)C44—C43—C42122.2 (11)
C7—C8—H8A120.1C44—C43—H43A118.9
C3—C8—H8A120.1C42—C43—H43A118.9
C10—C9—C6175.6 (10)C43—C44—C45117.9 (10)
C9—C10—P2i172.5 (9)C43—C44—H44A121.0
C16—C11—C12119.8 (8)C45—C44—H44A121.0
C16—C11—P1121.5 (7)C44—C45—C46121.6 (10)
C12—C11—P1118.7 (7)C44—C45—H45A119.2
C13—C12—C11119.9 (9)C46—C45—H45A119.2
C13—C12—H12A120.1C41—C46—C45118.7 (10)
C11—C12—H12A120.1C41—C46—H46A120.6
C14—C13—C12119.6 (10)C45—C46—H46A120.6
C14—C13—H13A120.2Cl2—C1S—Cl1108.6 (5)
C12—C13—H13A120.2Cl2—C1S—Cl3110.6 (6)
C13—C14—C15121.1 (9)Cl1—C1S—Cl3111.2 (5)
C13—C14—H14A119.4Cl2—C1S—H1SA108.8
C15—C14—H14A119.4Cl1—C1S—H1SA108.8
C16—C15—C14119.1 (10)Cl3—C1S—H1SA108.8
C16—C15—H15A120.5C2Sii—Cl5—C2S33.7 (14)
C14—C15—H15A120.5C2S—Cl4—C2Sii33.6 (15)
C15—C16—C11120.5 (10)C2Sii—C2S—Cl5ii74 (2)
C15—C16—H16A119.8C2Sii—C2S—Cl473.2 (7)
C11—C16—H16A119.8Cl5ii—C2S—Cl4111.7 (10)
C22—C21—C26118.2 (8)C2Sii—C2S—Cl572.5 (17)
C22—C21—P1119.7 (7)Cl5ii—C2S—Cl5113.0 (10)
C26—C21—P1122.0 (7)Cl4—C2S—Cl5111.2 (10)
C23—C22—C21121.0 (9)C2Sii—C2S—H2SA179.2
C23—C22—H22A119.5Cl5ii—C2S—H2SA106.9
C21—C22—H22A119.5Cl4—C2S—H2SA106.8
C22—C23—C24119.8 (9)Cl5—C2S—H2SA106.8
Symmetry codes: (i) −x+3/2, −y+1/2, −z+1; (ii) −x+2, y, −z+3/2.
Acknowledgements top

The authors acknowledge NSERC Canada and the University of Toronto for funding.

references
References top

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